Electrically conducting coated glass or ceramic article suitable for use as a lens, a window or a windshield, or the like



NOV- 28, 1961 w. H. coLBERT 'E1-AL 3,010,850

ELECTRTCALLY DUCTING COATED GLAss oR CER c ARTICLE su LE FOR usE As A LENs, A wTN w A wTNDsHTELD, 0R THE LIKE OR Original Filed Oct. 29, 1952 2 Sheets-Sheet 1 Fl G2.

' INVENT WILLIAM H. BE By AR R R. NRICH Wl RD L. MORGAN ATTORNEYS Nov. 28, 1961 w. H. coLBER-r ETAL ELECTRICALLY CCNDU COATED CLAss 0R CERAMIC ARTICLE sa A LENS, A wINDow SUITABLE OR A WINDS LD, OR THE LIKE Original Filed Oct. 29. 1952 2 Sheets-Sheet 2 IN V EN TORS WILLIAM H.C0|| BERT y ARTHUR n wElNRlcH wlLLARD L .MoRGAN ATTORNEYS United States s 01o sso ELECTRICALLY CoNbUrrNG COATED GLASS on CERAMIC ARTICLE SUITABLE Eon USE AS A LENS, A WINDOW R A WINDSHIELD, OR THE LiKE 12 Claims. (Cl. 117-211) The present invention relates to electrically conducting coated glass or ceramic articles suitable for many uses, including light transmissive electrically conducting optical articles such as a lens, a window or a windshield, or the like, which are unique in that they are coated with a highly transparent electrically conducting coating, and including other articles of transparent or substantially non-transparent nature such as space heaters, electrical resistances and conductors,'static dissipators, light transparent radio frequency shields, and at conductors useful for producing electrical iields.

The articles comprise a body of glass or other ceramic material of siliceous nature which may be transparent or opaque in which a continuous layer is formed upon such body by depositing thereon by molecular deposition within a vacuum either by thermal evaporation or by sputtering an intimate -molecular mixture of a metal and a metallic inorganic dielectric compound, and in a layer whzh is substantially uniform in thickness and the proportion of metal to the dielectric compound in such layer and the thickness of said layer are such that said llayer is electrically conductive. By such a construction it has been found that not only are products produced which are strongly adherent and durable, but they are of a maximum light transmission when so desired yand of a very high degree o-f electrical conductivity when even very thin films of the intimate mixture of metal and a dielectric compound are thus used.

The application of products having both electrical properties and light transmissive or other optical properties such as reflection or specific opacity to electrical waves or various parts of the visi-ble spectrum calls Ifor a careful designing of the products to each particular problem. More important, since most electrical problems involve the specific requirements of certain energy flows at very specilic voltage or current requirements, the products generally have to be built to la specific or limited range of electrical conductivity or electrical resistance as defined by over-all ohms resistance for a certain length, or more particularly, by the factor of ohms per unit of square area in dealing with the flat areas such as in many of the products herein described.

It is one of the advantages of the present invention that products of an extremely wide range of electrical properties varying in electrical resistance from a few ohms per square up to a value -approaching the conductivity of uncoated glass (approximately 1200 megohms) may be readily prepared as stable articles in which the value of resistance may be controlled with great accuracy.

Thus, in the production of static dissipating coatings, such as those suitable for instrument faces or transparent work table tops, it is merely desirable that these be capable of carrying relatively small currents of a few milliamperes only and the electrical resistance may generally be of most any value. On the other hand, if such a static dissipating coating is to be employed upon a window or airplane canopy, it is generally desirable that such window be also transparent both to light and to radio frequency signals and in such cases the electrical ice conductivity should be held well above 50,000 ohms per square. Conversely, it is apparent that -for shielding radio frequency such as may be generated in an ordinary fluorescent lighting tube it is desirable to have aV highly light transparent electrically conducting coating which i's also very highly conductive for electricity and in this case it would be desirable that the coating vlbe of less resistance than 1,000 ohms per square.

The present invention also relates particularly to the production o-f a novel type of windshield -or window, or other transparent optical articles such as a lens or 4goggle which maybe electrically heated -by passage of current through the electrically conducting transparent coating deposited thereon. In such articles, and also in the case of space heaters such as may be employed in walls of buildings as over-all heat radiators which of course need not be transparent, there 'are very high requirements for electrical conduction and in these cases it is highly desirable that the electrical resistances be lower than 200 ohms per square and as low as a few ohms pervsquare. However, in these cases, as well as in the forming of flat or contoured glass or ceramic bodies, having electrically lconductive coatings thereon 'employed for the purposes of setting up electrical fields, a specific electrical conduction or electrical resistance value is generally desired dependent upon the voltages available in such installations and the actual current iiows desired.

Attempts to prepare electrically conducting articles, and particularly transparent electrically conducting articles, by deposition, by thermal evaporation in a vacuum, or by sputtering have not bee-n successful Where it has been desired to have a product of over 5,000 ohms per square since in order to secure such high resistances the metal coatings had to be of only a few molecules thick-ness and the inventors have found that when such coatings of less than Angstrom units or 25 molecules thickness were prepared, that it was impossible to secure duplicable results and that the values of electrical resistance secured were extremely high and extremely variable. Such products also lacked generally any hardness or resistance to wiping off from the siliceous or glass surfaces since the metals employed did not stick directly tosuch surfaces. Where it was desired to produce products of relatively high conductivity or lower ohms Vresistance than the 5,000 ohms per square figure given, it was found that again, the failure of the metal to stick to the siliceous surfaces prevented a production of reproducible products and led to extremely erratic results in -electrical conductivity and also in light transmission.

The present application is a division of `our prior co pending application Serial No` 317,472, filed October 29, 1952, now United States Patent No. 2,852,415, which is a continuationin-part of our` prior application Serial No. 88,208, filed April 18, 1949, now United States Patent No. 2,628,927, which in turn is a continuation-inpart of our prior application Serial No. 541,964, filed lune 24, 1944, now Unite-d States Patent No. 2,482,054.

In our prior Patent No. 2,628,927 the inventors have disclosed one means of preparing electrically conductive articles particularly of a transparent nature in which the desired adhesion and resultant durability were secured bly depositing first upon the siliceous surfaces a uniform continuous coating of a metallic inorganic compound such as ya metal oxide, metal sulfide, or metal halide. Upon such coating there was then deposited a metal layer and when the metals were deposited upon such metallic compound surfaces they were found to give continuous uniform metal layers which were highly adherent to the metal compound and in turn to the glass or siliceous surfaces. By the use of such metal compound layers upon the siliceous surfaces it was found possible to deposit metal coatings which were extremely thin but which were continuous'and uniform in nature in ycontrast to the erratic results resulting from direct deposition upon the uncoated siliceous surfaces where these continuous coatings were secured.

In the present invention there is formed a continuous layer which consists of an intimate molecular mixture of a metal and of a metallic inorganic compound. ln some cases this layer may be deposited directly upon the surface of a support body or in some cases it may appear as an intermediate layer in a composite structure. The inorganic metallic compoundvprovides .adhesion between the mixed composition layer and the siliceous support and also provides adhesion to themetal which is molecularly mixed throughout withthe inorganic compound. For such compositions it is found that the products are strongly adhered to the supports and are durable and hard, and that as the metal atoms are deposited in the intimate molecular mixture with the metallic inorganic dielectric compound that they are not free'to move and are located in such mixture in accordance with the manner in which they are laid down by the molecular deposition method of either thermal evaporation within a vacuum or by sputtering under certain circumstances.

Lt would be expected that when a metal which is in itself electrically conducting and when a metallic inorganic dielectric compound which in itself is non-electrically conducting, are deposited as a mixture that the nonelectrically conducting dielectric would cause the product to be non-electrically conducting. It has been found however, that when such a mixture is formed in which the mixture is an intimate molecular mixture where the materials are essentially present in molecular condition that there is considerably more electrical conductivity than might be otherwise expected and it is presumed that there must be some method of conduction across the extremely small insulating spaces provided by the separating of the metal molecules from each other by the insulating but very small metallic inorganic dielectric molecules.

While the conductivity secured from a given amount of metal when mixed in such intimate molecular mixture with a metallic inorganic dielectric compound, is not as large as itrwould be if the metal were present as a continuous solid metal layer, this results in providing one of the advantages of the present invention. For certain higher resistance films consisting of pure metal the thickness of the iilms was necessarily very low, such for example as less than 100 Angstrom units, or in some cases less than 2O Angstrom units. It is an advantage in the present methodthat much more material is required to secure a given degree of electrical conductivity and the films are thereby thicker and thereby more durable and wear resistant. Thus, it is possible to prepare for the first time stable high resistant coatings in which a small amount of metal is dispersed in a relatively large amount of metallic inorganic dielectric compound and thereby a fairly good thickness of -hard durable nature may be employed. Thus,V attempts to prepare high voltage static dissipators in the past by the use of coatings of metal of less than 20 Angstrom units or greater thicknesss were generally highly unsuccessful due to erratic values, unstable electrical character, and lack of resistance to rubbing of such extremely thin films. The

method provides also the further advantage that metals subject to air oxidation or corrosion such as aluminum or silver, can be readily employed in that embedding vsuch metal atoms in the dielectric results in protecting them from change under ordinary atmospheric conditions.

It is apparent that the embedding provides coatings which are of improved hardness as compared with those secured where the relatively soft metals such as gold or aluminum are used as separate layers. Itis also apparent that with the metals molecularly dispersed with the dielectric that the metal atoms are fixed in denite position and are not free to diuse around so that the products show immediate stable' electrical values which do not change in storage nor readily change when the products are heated.

A further advantage coming from the present method and residing in the product produced is found in that by being able to incorporate t-he metal conductor into the dielectric as one layer it becomes possible to eliminate one interface which would be present if a continuous solid metal conducting layer was employed in the structure. lt is thus possible to build electrically conducting light interference operating coatings without a separate discrete metal conducting layer which would introduce optical problems at its own interfaces. Thus, the present method permits constructing optical light interference filters and mirrors or dichroic mirrors or lilters of a simplified construction.

The present invention may employ a continuous electrically conducting layer which consists of an intimate molecular mixture of a metal and metallic inorganic dielectric compound in which the proportion of the metal and metallic inorganic dielectric compound are substantially uniform throughout the layer. It may on the other hand employ such a continuous electrically conducting layer in which the proportion of metal and metallic inorganic dielectric compound varies continuously throughout its depth in actual ratio of the two or more materials.

The invention alsol comprises the use of such a continuously varying blending mix layer in which at one interface of such layer it is in contact with substantially pure metal and the layer changes from thereon by an increasing amount of dielectric up to the point where at the otherinterface the composition becomes practically pure dielectric. The invention also conceives the use of such a graded layer which is electrically conducting in itself as an intermediate layer which also operates to adhere an electrically conducting layer of pure metal either directly to the siliceous support or to a preceding coating, and also such mixed layers, that will serve as adhering layers between an underlying electrically conducting layer and adhere it to an overlying protective layer such as one of silica. In such constructions the mixed metal and dielectric layers operate not only from an adhesion functioning but from an optically 4functioning and from an electrically conducting functioning also in addition to thatof the pure metal layer. Thus, it lwill be apparent that such a mixed metallic inorganic dielectric and metal layer, while primarily functioning as an adhesion layer to adhere a pure metal layer to some other film or support, will be in itself electrically conducting and will further provide the interesting optical feature Athat Where it is graded from pure metallic inorganic dielectric in contact with the surface to which adhesion is to be secured, through a graded composition to a place where it is in contact with pure metal and is substantially pure metal, then the optical result is secured that an optical face between such graded mixed electrically conducting layer and the pure metal layer is avoided. Similarly, it is possible by the present method to also avoid an optical interface between a pure dielectric coating and the mixed electrically conducting layer where such is graded from pure dielectric in the mixture in contact with the pure dielectric nlm and vby grading through an increasing amount of metal into contact with the pure metal, both optical interfaces may be avoided.

It will be apparent that depending upon the relative amounts of metal and metallic inorganic dielectric employed and the volumetric ratios between atoms of such materials, that the electrically conducting layers may in some instances have metal atoms which are surrounded substantially by dielectric atoms and in other cases may have dielectric ato-ms substantially surrounded xby metal atoms and it is apparent that both such instances may occur within any particular lilm regardless of a relative volumetric composition. Thus, at best, the conduction would seem to be .through small chains of a few metal atoms in contact and across insulating spaces where the dielectric breaks such possible direct contacting metal atoms. At any event it is apparent that the conductivity through such a film must be by some tortuous path and that the resistance to be secured would normally be higher for a given amount of metal than would occur if the same amount of metal was present in a uniform continuous solid film by itself. Thus, it also is apparent that in order to secure a desired amount of conductivity more metal must be employed than would be the case where two separate layers were employed, one of which was a metal compound and one of which was metal, `as in our prior Patent No. 2,628,927. This greater thickness of metal and consequent carrying amount of dielectric results in the conducting layers in the products being thicker than those secured in the preceding invention. By this invention we cannot only prepare transparent electrically conducting articles as disclosed in our prior application, but the present invention permits the forming of articles of any desired transparency or opacity and lof any desired electrical conductivity.

It will be obvious that in forming an electrically conducting article in which the electrical conducting film is so extremely thin, it becomes very necessary that the coating be uniform in thickness as otherwise slight variations in thickness will result in variable electrical conductivity over the surface and development of greater heating at points of minimum thickness. Such development of hot spots may lead to burning out of such a film. In order to secure the necessary smooth continuo-us and uniformly thick conducting films, we prefer to deposit such electrically conducting coatings by molecular deposition such as thermal evaporation or sputtering. In the carrying out of such a method the metal may be evaporated from a filament or fiaments properly spaced and loaded and as such metal is evaporated thereV may be simultaneously and concurrently evaporated from another filament or filaments properly spaced and loaded a charge of the dielectric so that the t-wo materials are ointly and continuously deposited upon 4the support at the same time. When this is done 'and care is maintained that the two evaporations take the same time, the products wil be substantially uniform in composition throughout. The thermal evaporation may also be carried out where the two materials, namely the metal and metallic inorganic compound are mixed together in a predetermined weight ratio and directly evaporated from the same filament. If the materials are of approximately the s-ame evaporation rate properties, the film may be suhstantially uniform, and if they vary somewhat in rate of evaporation characteristics it is obvious that a graded film will be produced in which the faster evapo-rating material comprises a larger ratio of the first part of the film formed and a decreasing proportion of the film as it is progressively built up, and that the result is a graded film. Of course, such gradation within a film is subject not only to the relative evaporation rates and relative filament temperatures in such a case, but Ialso is affected by the relative amounts of each material applied to the filaments, or applied in the mixture which is supplied to the filament.

As a further means in which we may produce our layers includinfy dielectrics comprising metallic oxide we may proceed by thermally evaporating in a vacuum a mixture of two metals, one of which is relatively easy to oxidize such as aluminum, and one of which is relatively diiiicult to oxidize such as gold, and thereafter oxidizing this mixture by heating 4the deposit at an ele vated temperature in the presence of oxygen to convert the one relatively easily oxidizable metal to an oxide. Obviously, other oxidizable materials such as the metallic sulfides, might also be converted to oxidized metallic compounds by heating the glass or other support which -6 is precoated with the relatively non-oxidizable metal and metallic sulfide in a furnace to a high temperature in the presence of oxygen to convert the dielectric sulfide to a dielectric oxide in the electrically conducting mixed film.

A further way in which thin layers of metal land of metal oxides specifically may be produced in position upon a glass or other support is to proceed by applying a thin coating by sputtering `a metal in a residual vacuum suitable for sputtering, in which the residual vacuum comprises in part oxygen such `as from evacuating an air filled vessel. This sputtering may he carried out in methods well known in such art, employing the metal which is to be sputtered as an electrode; and in some cases where a metallic evacuation chamber is employed and this is used as one of the electrodes, a coating of the metal which is to be sputtered is first applied to the chamber walls. The latter is particularly advantageous where an AC. rather than a D.C. current is employed., In such cases the other electrode would preferably be of the metal desired to be sputtered. Thus, if copper is sputtered in the presence of residual air, copper oxide deposits are formed upon the glass, and the coatings thus produced are extremely adherent to the glass. If the amount of residual oxygen is decreased by the injection into the chamber of inert gases it is possible to produce by sputtering in such a reduced oxygen atmosphere mixtures of copper and copper oxide. Surprisingly also, when the metals silver, gold, platinum and palladium, which are resistant to oxidation, lare sputtered in a residual oxygen system it is found that the deposits are to a very large degree composed of oxides of these metals. By such a method then, it is possible with these metals, silver, gold, platinum and palladium, to produce electrically conducting layers 'of these metals with their oxides in intimate molecular mixture.

In view of the foregoing general remarks, it is an object of the present invention to produce an electrically conducting layer which is characterized by its electrical stability, its hardness, its ability to adhere to siliceous or other support surfaces, and by the fact that the layer may ybe accurately controlled as to electrical resistivity both in extremely low and extremely high ranges.

It is a further object of the present invention to provide an electrically conducting layer of the character described which comprises an intimate molecular mixture of metal and an inorganic dielectric metallic compound.

It is a further object of the present invention to provide an electrically conducting layer of the character described in the preceding paragraph in which the mixture of metal and dielectric metallic compound is substantially uniform throughout.

It is a further object of the present invention to pro vide an electrically conducting layer of the character described above in which the proportion of metal and dielectric metallic compound is selectively varied from one surface of the layer to the other.

It is a further object of the present invention to provide an electrically conducting layer which comprises an intimate molecular mixture of metal and an inorganic dielectric metallic compound, which is characterized by substantial thickness while having an electrical resistivity which may be in an extremely high range.

It is a further object of the present invention to provide an electrically conducting partially transparent layer comprising an intimate molecular mixture of a metal and an inorganic dielectric metallic compound.

It is a further object of the present invention to provide an electrically conducting layer in which the elec- -trical resistivity may be controlled as desired between extremely low and extremely high ranges which may be useful in such varied products as electrically heated windows, windshields or the like, electric goggles, electric resistance units, electrostatic dissipators, radio frequency shields, space heaters, and the like.

It is a further `object of the present invention to provide an electrically conducting -layer comprising a mixture of metal and inorganic dielectric metallic compound which may be used as an intermediate graduated adhesive layer for adhering a metallic film to a support surface without producing an optical interface between the adhesive layer and the metallic film, and which may also avoid the occurrence of an optical interface provided the dielectric compound in the layer is substantially optically identical with the material providing the support surface.

.It is a further object of the present invention to provide a novel method of producing electrically conducting layers as described in the preceding paragraphs.

It is a further object of the present invention to pro vide an approximately transparent electrically conductlng layer useful in interference mirrors, dichroic filters and light transmissive radio frequency filters.

It is a further object of the present invention to provide a method for producing electrically conducting layers as described in the preceding paragraphs in which a metal and an inorganic dielectric metallic compound are deposited by molecular deposition simultaneously and concurrently on a support surface.

It is a lfurther object of the present invention to provide a method of producing an electrically conducting layer as described in the preceding paragraph in which the metal and dielectric compound are provided in the form of a mixture and are evaporated either simultaneously and concurrently or in an overlapping sequence from a single filament.

It is a further object of the present invention to provide a method for producing electrically conducting layers of the character described in which the -metal and the dielectric metallic compound are evaporated either simultaneously and concurrently or in an overlapping timed sequence from separate filaments.

It is a further object of the present invention to provide a method for producing electrically conducting layers as described above in which a metal is sputtered in a residual vacuum containing oxygen and in which the metal is either of a group relatively difficult to oxidize or in which the amount of residual oxygen is controlled so as to prevent complete oxidation when the metal is relatively easily oxidized.

It is a further object of the present invention to provide a method for producing electrically conducting layers of the character described in which a mixture of a plurality of metals, one of which is relatively dii'licult to oxidize and another of which is relatively easy to oxidize, are deposited as an intimate molecular mixture on a support surface, subsequent to which the deposited layer is heated in the presence of oxygen under conditions which will produce oxidation of the metal relatively easily oxidized while preventing substantial oxidation of the metal which is relatively difcult to oxidize.

Other objects and features of the invention will become apparent as the description proceeds, especially when taken in conjunction with the accompanying drawings, wherein:

FIGURE l is a fragmentary sectional view showing a layer constructed in accordance with the present invention applied directly to a support body, for example a siliceous body, such for example as glass, and having electrodes applied to the opposite ends of the electrically conducting layer.

FIGURE 2 is a fragmentary sectional View of an electrically conducting beam splitter or dichroic mirror.

FIGURE 3 is a fragmentary sectional View illustrating the use of our electrically conducting layer as an intermediate layer between a dielectric layer and a metdlic layer and in which suitable electrodes are shown.

FIGURE 4 is a fragmentary sectional view of an electrically conducting Window suitable for use in a vehicle or optic goggles.

FIGURE 5 is a fragmentary sectional view of an electrically heated lens or goggle.

FIGURE 6 is a fragmentary sectional view through a double glazed window, one pane of which is pro-ved With the electrically conducting film.

FIGURE 7 is a fragmentary sectional view through a laminated glass article such for example as a windshield, one ply of the glass having the electrically conducting iilm applied thereto,

FIGURE 8 is a diagrammatic view illustrating a Windshield and showing the manner in which the electrical circuit is completed through the electrically conducting film.

FIGURE 9 is an enlarged fragmentary sectional view on the line 9 9, FIGURE 8.

FIGURE l0 is a sectional view through a double convex lens having an electrically conductive film applied to the opposite sides thereof so that the lens may be employed as a magnetic shutter in a polarized light system.

FIGURE ll is a front elevational View of an electrically conducting film or layer applied in a definite pattern to a portion only of the surface of a support body.

The present invention deals With the provision of an electrically conducting film or layer comprising an intimate molecular mixture of a metal and an inorganic dielectric metallic compound.

As the metals to be employed in forming the electrically conducting films with the dielectrics there may be employed any solid metal which may be thermally evaporated in a vacuum or sputtered. Thus, We may for example, employ copper, gold, silver, aluminum, platinum, rhodium, nickel, iron, cobalt, tin, titanium, cadmium, zinc, chromium, manganese, palladium, magnesium, zirconium, vanadium, lead, arsenic, antimony, and bismuth. 'I'here may also be employed under special circumstances Where the product is isolated in a dry atmosphere or Vacuum such metals as sodium or calcium.

As the inorganic dielectric metallic compounds there may be employed such metallic compounds as metallic oxides, metallic suliides, or metallic halides, or a metal sulfate or other stable dielectric metallic compounds. We have found that the met-allie oxides such :as those of lead, silver, aluminum, magnesium, zinc, and other rare earth metal oxides, and the oxides of cadmium, antimony, bismuth, mercury, copper, gold, platinum, palladium and other heavy metal oxides, when applied over glass or other siliceous surfaces, are extremely highly adherent to such surfaces and that furthermore, they are highly adherent to the metals. Such oxides may be employed mixed with the metals to produce our electrically conducting layers. We have also found that other metallic compounds may be used as the dielectric with the metal in forming our electrically conducting films. Thus, as metallic compounds that are generally highly effective We may use the sulfides, selenides, tellurides, sulfates, selenates, tellurates, halides such for example las fluorides, or other compounds relating to the metallic oxides which we have indicated above and derived from the indicated metals. More particularly, We have found that the inorganic metallic compounds of any metal in the form of a sulfide, selenide, telluride, sulfate, selenate, or tellurate, or the halides of such metals may be employed. The choice Vof a specic metallic dielectric Will of course be dictated by other considerations such as Water insolubility, light stability, and ability to evaporate the material or to form it upon a glass surface in a vacuum chamber operation. For example, as suliides We might readily use as our dielectric a deposit of a sulfide of antimony, lead, zinc, cadmium, tin, arsenic, bismuth, iron, nickel, cobalt, copper or silver. These would be generally useful. We might also use the sulfides of sodium, potassium, or calcium but in such case the product would have to be one where the coating Was sealed within a vacuum continuously since such coatings are rapidly destroyed by absorption of moisture when directly exposed to air. That is, these materials are suitable in dry evacuated systems but are not useful in products exposed to air. On similar consideration we have found the use of lead selenide, lead sulfate, lead telluride, and lead tellurate as being of particular use in forming the desired coating.

While most sulfates are water soluble, lead sulfate is quite non-soluble and can be used to secure good stable products for use in ordinary atmospheres. While all metallic sulfates and inorganic metallic sulfates might be employed, it is obvious that where we employ a water soluble one such as zinc sulfate, that the layer should be kept within a dry water-free atmosphere or in a vacuum since water absorption will cause loosening of the coating.

As suitable metallic halides there may be employed lead bromide, lead chloride, lead uoride, lead iodide, or silver chloride. While all metallic halides or compounds of a metal with an element of the halogen family, namely, brornine, chlorine, fluorine, or iodine, may be employed, it is obvious that those just listed have the advantage of being stable to light, and of being water insoluble. It would be obviously possible to use light sensitive halides such as silver bromide in a transparent electrically conducting structure in which an amber or ultra violet opaque glass was employed in which the amber protected the halide from the photochemical action. However, it is possible to use water soluble materials such as sodium chloride, sodium fluoride, chromium iluoride, magnesium chloride, calcium chloride or iron chloride', if the coated articles which are produced' are maintained in a dry atmosphere or in a vacuum so that the coatings are protected against absorbing water and loosening from the glass by the water soluble metallic halide being displaced from the glass surface. `Other suitable water insoluble metallic fluorides which may be employed yare magnesium uoride and lithium tluoride.

There may be also employed other suitable dielectrics such as magnesium silico-lluoride. We may also employ mixed oxides or compounds of these such as the spinels, as the dielectric. For example, a molecular mixture of magnesium oxide and aluminum oxide or the ordinary socalled spinel may be employed as the dielectric. It is also within the scope of the present invention to employ more than one dielectric, provided one is an inorganic metallic compound, within any given layer and it is also obvious that our electrically conducting layers might be made where more than one metal is employed in the composition, such mixed metals constituting an approximation to known alloys such as copper and nickel in a ratio similar to Monel, or for example the nickel chromium mixture known as Nichrome. With these particular alloys one can secure such ratios of the metals present readily by directly evaporating such alloys as they distill in thermal evaporation without any substantial composition change.

Inasmuch as the electrically conducting ilm or ylayer disclosed herein is of a thickness such that it is not selfsupporting and cannot be used apart from supporting structure, it will normally be applied to a supporting body, either directly to a surface of the support body or to the surface of a previously applied layer or coating. In some cases opt-ical properties of the resulting body are sigm'cant in which case the surface of the support to which the layer is applied will be an extremely smooth surface such as a polished glass surface. Such would be the case for electrically conducting vehicle windows or optics. However, where the resulting article is to be employed by virtue only of its electrical properties, the surface need not be smooth or highly polished and excellent results have been obtained when the layer has been applied to a porous ceramic surface.

It will be appreciated that the electrical resistances given in the following examples and mentioned throughout this speciiication are given as ohms per square area and that such electrical resistivities are as usual, the reciprocals of electrical conductivity, thus, the lower the electrical resistance the better the electrical conductivity,

Vand if a ilm has an electrical resistance of ohms per square it has such a resistivity regardless of whether the square is one inch on the side or one foot on the side. In applying the products of the invention to specific applications the desirability of securing very low electrical resistance or high electrical conductivity becomes emphasized in the choice of voltage at which the electrically heated Window or lens, etc., must be operated in order to provide such ener-gy. The voltage E required to supply a given amount of energy W to a square of ltreated glass one square foot in area, .when the current is applied to asquare of glass, can be determined by the following simple formula in which R is indicated as the electrical resistance.

Furthermore, within the limits permitted by a specic application, itis of course best to maintain a window to a minimum width in one direction since by elongating Vin the other and attaching the electrodes along the long edges, one secures the advantages of having a number of resistances thus connected in parallel.

Lenses employed in the goggle of a helmet used in cold or freezing weather have always been subject to clouding up due to condensation and freezing of the breath upon the same, and the initial transparency of the glass 'is rapidly destroyed. In airplanes and other fast moving vehicles such as trains which are moving through cold strata of air, there exists a very serious problem of condensation of moisture, or under more severe conditions, actual ice formation upon the Windows of the vehicle. In

4the case of airplanes the icing of the windows has presented a very yserious problem. If heat could be applied to such surfaces during use the objectionable clouding and freezing over might be eliminated, but the application of heat as such directly cannot normally be conveniently carried out. The articles prepared in accordance with this invention carry an electrically conducting coating thereon which permits the direct generation of heat in contact with the glass, light transmitting windows, or viewing lenses at all points over the surface of such glasses. In the determination of the necessary amount of heat which must be brought to a glass surface to prevent icing, for example in an airplane, it is found that a tremendous amount of heat such as between 2,000 and 4,000 British thermal units per square foot per hour must be supplied. To supply so much energy to a square foot of glass surface continuously requires a very eiiicient means of producing the heat directly in contact with the glass so that the heat may be carried through the glass to the front surface exposed directly to the cold atmosphere or directly developed on such front exposed surface. This large amount of heat when considered in terms of the amount of electrical energy which must be supplied, for example to a windshield four feet by one foot, runs into some 4,000 watts and from such a figure it immediately becomes apparent that for any conductor to be applied to the surface of the glass to heat the same and supply such an amount of energy, the conductor must be one of a very high degree of conductivity.

Experience has indicated that the electrical resistivity of such an electrically conducting lm should be less than 100 ohms per square and at all events, not more than 150 ohms per square. At the same time experience has shown that for transparent closures suitable for a windshield and the like, a light transmission of not less than 50% is essential. In fact, it is a present requirement of windshields that they shall transmit at least 70% of normally incident light. Accordingly, in the present invention the light transparent electrically conducting film, when used as a windshield, is preferred to have an electrical resistivity of not more than ohms per square while preserving alight transmission property of not less than 5 0% vand preferably of not more than 100 ohms and a relatively high light transmission of not less than 70%.

t1 i Y Thus, in the case of an airplane it has been estimated that it is necessary to supply between 2,000 and 3,000 British thermal units per square foot per hour, or an average of 800 watts per square foot to the window to prevent icing. if 800 watts per square foot are to be ygenerated within a glass having a resistance of 100 ohms when current is passed across a one square foot piece, the voltage required would be 283 volts. Since in moving vehicles it is highly advantageous to avoid electrical circuits which involve high voltages due to the danger inherent in accidents or particularly inherent in short circuits developing in wet weather, it becomes highly desirable that any electrically conducting glass to be used in a moving vehicle be not substantially of greater resistance than this ligure, and in all events have a resistance per square of not more than 150 ohms, and in general it is desirable for the resistance per square to be yat a lower value to thereby permit operation with reduced voltages. It will be obviously apparent that the requirements for heat upon an automobile or train windshield be far less than that required for an airplane, estimates ranging from 50 to 75 watts per square foot, and that consequently the articles of this invention may be employed upon such vehicles at reasonable voltages.

With a man walking in a minus 60 degrees Fahrenheit temperature with a helmet employing a partially transparent lens of the invention of three square inches, the heat demand to prevent fogging and icing has been estimated at around 1 watt per square inch. With such a lens of square shape and 1.7 inches on a side and l ohms resistance, a voltage of only 6 volts is necessary,

which may conveniently be supplied by a small dry cell battery or hand operated generator.

Referring now to the drawings, in FIGURE l there is illustrated a support body 10 which in the present case may be a transparent or opaque body and which may be this figure may be of uniform composition or variable composition. Electrodes 13 are shown at each end of the layer as means of passing current through the film.

In FIGURE 2 there is shown a construction which is both electrically conducting and partially transparent and partially reflecting which maybe employed as a beam splitter to thus separatev light into two different paths.

The product approximately splits light into approximately two equal beams by rellection and transmission with some absorption loss where the three separate layers are each ,approximately one-quarterY wave lengththick as referred "to visible yellowV light of 5500 Angstrom units.

In the iigure 14 is a transparent glass support, 16 is a layer of titanium dioxide applied thereto by thermal evaporation from a iilament, and layer 18 is a successive layer applied on layer 16 by thermal evaporation of magnesium uoride. Subsequently, in the same vacuum there was evaporated from a third lilament a mixture of 20% metallic titanium and 80% of titanium dioxide by weight. This top layer 20 was electrically conducting and provided the article with such properties, the conductivity being 100,000 ohms per square area. A modiiied form of the same product which has the property of selectively rellecting a high amount of blue lightand selectively transmitting a high amount of the remainder of the visible spectrum or amber light is made in the same manner with the same three types of layers with the exception that each layer is made to be a quarter Wave length of light with reference to 4,000 Angstrom units blue light. The product in this case is then a selective reflecting and transmitting dichroic mirror or lter which is at the same time electrically conducting and which may be used with cathode ray apparatus to prevent building up of static charges on such an optical unit.

In FIGURE 3 there is shown a variation of the present invention in which the film or layer comprising a mixture of metal and the dielectric material is disposed intermediate an adhesi-ve layer and a layer composed of pure metal. In this figure a support body is illustrated at 22 and again may be a glass body. Upon a surface of the glass body there is deposited a relatively thin adhesive layer 24 which may be composed of a metallic compound effective to adhere strongly to glass and to provide adhesion for subsequently applied layers. On the outer surface of the adhesive layer 24 there is deposited the layer 26 which comprises an intimate mixture of metal and the inorganic dielectric metallic compound. Finally, there is deposited the outer layer 2S which is in this case illustrated as a layer of pure metal. The layer 26 is a graduated layer in which the portion of the layer adjacent the surface of the adhesive layer 24 is composed entirely or almost entirely of the dielectric material. If the dielectric inorganic metallic compound material in the layer 26 is the same material which is employed as the adhesive layer 24, it will be appreciated that no optical interface exists between the layers 24 and 26 and accordingly, the boundary between these layers is illustrated in the present `figure asthe broken line 30. The proportion of metal to dielectric inorganic metallic compound material in the layer 26 increases progressively from the layer 24 to that portion of the layer 26 adjacent the metal film 28 and preferably, the outer portion of the intermediate lilm 26 is composed entirely of metal and in this case preferably of the same metal as occurs in the film 28. As a result of this there is no optical interface between the iilms 26 and 28 and accordingly, the boundary between these lms is indicated in the iigure as the broken line 32. As a result of the foregoing construction there is applied to the glass body 22 a metal film 28 which may be transparent, partially transparent, or opaque, and which has a conductivity substantially equal to the conductivity of the massive metal. At the same time the metal film 28 is adhered to the glass by means which avoids the occurrence of optical interfaces with resulting improvement in optical properties for certain purposes.

In FIGURE 4 there is illustrated an article comprising a support body 40 which may be a glass body. Applied to the outer surface of the glass body 40 is a hn or layer 42 which in the present instance is in intimate molecular mixture of a metal and an inorganic dielectric metallic compound. In the present case this mixture may be of uniform composition throughout or it may be of a gradually varying composition. Applied to the outer surface of the layer 42 is an intermediate film 44 of metal. Applied to the outer surface of the layer 44 is a film or layer 46, again comprising an intimate molecular mixture of a metal and a dielectric inorganic metal compound. In the present case an outer layer 48 is applied to the layer 46 and may comprise a layer of silica. In a specific example the layers 42 and 46 comprised an intimate molecular mixture of iron oxide and gold. The intermediate metallic layer 44 comprised gold. The article illustrated in FIGURE 4 is useful as an electrically heated windshield or the like.

Referring now to FIGURE 5 there is illustrated the application of the electrically conducting film to a goggle 50, the iilm being indicated at 52 and applied directly to the outer convex surface of the goggle.

In FIGURE 6 there is illustrated a portion of a double glazed window comprising panes of glass S4 and 56 connected along two opposite edges by metallic spacers S8, the spacers at the other two edges being of dielectric material. The' glass 56 is illustrated as having applied thereto a transparent conducting film 60 which is applied directly to the inner surface of the glass 56. The electrically conducting film 60 in the present instance is of course highly transparent and comprises an intimate molecular mixture of a metal and an inorganic dielectric metallic compound. Electric current is applied along opposite edges of the electrically conducting film 60 by suitable contacts which may be constituted by the metal spacers S.

In FIGURE 7 there is illustrated a windshield of the well known safety glass construction which comprises `outer and inner sheets of glass indicated at 62 and 64 respectively. These sheets of glass are assembled into a sandwich with an interposed layer 66 of a suitable plastic material such for example as polyvinyl butyral or other plastic of approximately a preferred refractive index of about 1.5. By the choice of plastic of such approximate refractive index, it is found that the refiection from the coated surface is decreased upon lamination. A highly transparent electrically conducting film 68 is carried by the inner surface of the glass sheet 51 and is adhered thereto. With the parts in the relationship illustrated in this figure the windshield is designed for use with the glazed sheet 62 as the outer or forward sheet of a windshield.

Referring now to FIGURE S there is diagrammatically illustrated the manner of providing an electric circuit for a windshield. In this case elongated contacts 70 and 71 are provided along the long edges of the Windshield 72, it being understood that the windshield 72 is provided with a transparent electrically conducting film of the type disclosed herein. An external source of current is indicated at 74 for connection by conductor 75 Vto the contacts 70 and 71, thus causing the current to traverse the metal film of the windshield.

In FIGURE 9 there is illustrated an enlarged section of FIGURE l() showing the manner of attachment of a contact S0 to the electrically conducting film 68 which may be that illustrated in FIGURE 7. In this case the electircally conducting film 68 is adhered to the glass sheet 62. The glass sheet 62 is assembled with the glass sheet `64 by the intermediate ply of plastic 66 as described above. In order to provide a good contact between the contact element 80 and the electrically conducting film 68, additional metal is provided as indicated at 82. This may be done by additional thermal deposition of material along the edges of the article or it Vmay be applied otherwise, such for example as by spraying. Such metal for contacting may also be applied in any of the present products by directly electroplating metal on the desired portions using masking protective lacquer coatings to protect the main face of the product desired to be free of such electroplated electrode areas. The electroplating current is fed directly into the first produced electrically conducting layer of the invention. In this figure .contact 80 which may be a strip of thin copper, has its edge embedded in the plastic material 66 and is retained in firm pressure contact with the metal 82 in the final assembly. The electric leads to the source of current may be applied to the contact 80 at the face of the glass.

In FIGURE l0 there is illustrated the application of the electrically conducting films 90 to both sides of a double convex lens 92. It will be understood that in this case the electrically conducting films are adhered directly to the surface of the glass. In this figure there is also illustrated electrical contacts 94 and 96 for supplying current to the electrically conducting coatings. It will be understood that the contacts 94 and 96 are provided in the form of arcs of circles having portions extending in area contact with peripheral portions of the electrical conducting films and that the contacts 94 and 96 are separated from each other and that the current is completed between the contacts 94 and 96 through the electrically conducting films 90.

In FIGURE 11 there is illustrated another application of the present invention in which the electrically conducting film is shown at 100 as applied in the form of a pattern to a support body such for example as a window pane 162. In this case the article may be useful as a burglar alarm, interruption of a current passing through the electrically conducting film by breakage of the glass being effective to actuate an alarm.

We have found that there are practically no adhesional forces between metals and glass or siliceous surfaces, as can be seen when adhesive tape is applied directly to metal coatings which are directly applied to glass. When stripping the tape the metal will strip off very readily. This was one of the difculties in attempting to prepare electrically conducting articles. The articles produced under this invention will when subjected to the adhesive tape test, successfully resist any pulling away from the glass or siliceous surface showing that there are strong bonds between the surface and the electrically conducting layers.

The articles constructed in accordance with the disclosure herein, exhibited very great resistance to separation of the electrically conducting film from the support body and a suprising resistance to abrasion, and this is accomplished without in any way detracting from optical properties. The electrically conducting film is molecularly adhered to the siliceous support by the action of' the dielectric metallic inorganic compounds. Where a transparent or optical article is desired it is preferable that the surface be smooth, and by smooth surface we use the term in its ordinary sense. It need be only sufiiciently smooth to prevent visible or optical apparent light diffusion at such surface and sufficiently smooth to insure the avoidance of electrical hot spots by presenting a base upon which the electrically conducting film can be formed in a satisfactory layer. However, in many instances our invention can be formed on superficially rough ceramic bases. In the forming of articles by the present invention where the surface is smooth it is apparent that the Vsmoothness of the surface of the support body will be reproduced in the outer surface of the electrically conducting layer. Thus, if the smooth face of the support body is polished to have an extremely smooth finish this finish will be reproduced in the interfaces or surfaces presented by the electrically conducting layer.

It is one of the advantages of the present invention that electrically conducting'articles can be made upon optically `required surfaces Without destroying or altering such finer ground and polished faces.

Where it is desired that the electrically conducting film be both of a very high electrical conductivity and of a relatively high transparency, it is preferable that we employ gold, silver, copper, iron or nickel as the metal to provide the requisite combination of properties. It

'further becomes apparent that when we desire to make a window we also wish to avoid developing any reflection properties in such Window, particularly as for example in an automobile windshield where action of the windshield as a mirr-or would be highly undesirable. Generally speaking, we have found the use of gold to give us preferred products for use in windshields, windows and optical lenses by reason of this material providing highest light transmission with the highest electrical conductivity and at the same time, the lowest light refiection properties, and further, by reason of its cornplete inertness to oxidation or chemical change.

It will be apparent that the ldesired electrical conductivity in any product may be produced by altering either the total amount of metal and total amount of dielectric, or the ratios of these two materials to each other by Weight, or by altering the choice of dielectric and metal taken in forming the lm. Thus, the thickness, the composition, and the nature of components are the controlling factors in securing the desired electrical conducting, optical, and other properties of the products of the invention. Thus, it is possible in accordance with the present invention to produce an electrically conducting film having a high or even an extremely high resistivity approaching for example that of uncoated glass which may have substantial thickness and as a result of such thickness have substantial strength, durability, and hardness, and furthermore, as a result of such thickness being readily controllable as to the exact amount of its electrical resistance properties. Also, in accordance'with the present invention it now becomes possible to produce a lm of any predetermined thickness and having a definite predetermined value of electrical resistance. It is thus possible to product for example, a quarter wave length iilm which may have any -desired electrical resistance.

Examples 1, 2 and 3 From a lament there was evaporated in a high vacuum chamber 0.15 5 gram of copper and simultaneously, 0.155 gram of magnesium iluoride. contained 50% metal by weight and 25.5% by volume. The deposit was formed upon glass pieces placed separately at thirteen inches, seventeen inches, and twentyone inches away from the filament. The glass placed at thirteen inches had the thickest coating thereon and showed an electrical resistance of 20 megohms, or 20 million ohms, a light transmission of 56%, a reflection from the coated side of the glass of 14%, and through the glass the redectivity measured 6%.

The glass piece coated at seventeen inches showed an electrical resistivity of 200 megohms, a light transmission of 68%, la retiection from the coated side of 12%, and a redection through the glass of 5%.

The other glass, coated at twenty-one inches away from the iilament, showed an electrical resistivity of 1000 megohms, a light transmission of 78%, a reiiecton from the coated side of 10%, and a reflection through the glass of 6%. The coatings in each case were well mixed and were substantially uniform.

The copper deposited on the pieces of glass placed at thirteen inches, seventeen inches and twenty-one inches were respectively of a thickness of 126 Angstrom units, 74 Angstrom units, and 48.5 Angstrom units. In the same respective cases the thickness of magnesium iluoride deposits were 375 Angstrom units, 2li.l Angstrom units, and 144 Angstrom units.

The drawings and the foregoing speciication constitute a description of the improved electrically conducting coated glass or ceramic articles suitable for use as a lens, a window or a windshield, or the like, in such full, clear, concise and exact terms as to enable any person skilled in the art to practice the invention, the scope of which is indicated by the appended claims.

We claim:

1. An electrically conductive transparent article, com prising a body of sil-iceous material, a continuous tran-sparent electrically conductive layer carried by said body, saidlayer being deposited by molecular deposition and composed essentially of an intimate molecular mixture of metal and a metallic inorganic dielectric compound, in which said dielectric compound consists of a metal cation and at least one anion selected from the group consisting of brom-ine, chlorine, uorine and iod-ine, the layer being lsubstantially uniform in thickness, the proportion of metal to the dielectric compounds in said layer and the thickness of said layer being such that said layer is electrically conductive and serves to carry the major portion of electric current carried by said article.

2. An article as defined in claim l, in which the proportion of metal to dielectric compounds is constant throughout the layer.

3. An article as defined in claim 1, in which the proportion of metal to dielectric compound is variable throughout the layer.

4. An article as defined in claim 3, in which the pro- The mixture thusl Aportion of metal varies progressively from 0% to 100% from one surface ,of said layer to its other surface.

5. An article as defined in claim l, in which said layer is applied directly to a surface of said body.

, 6. An article as dened in claim l, in which said layer is an intermediate one of a plurality of layers applied to a surface of said body.

7. An article as defined in claim 1, in which said article comprises a second layer composed of the same dielectric compound as occurs in said tirst mentioned layer, and a third layer composed of the same metal as occurs in said first mentioned layer, said second and third layers contacting opposite surfaces of said rst mentioned layer, the proportion of metal to dielectric compound in said first mentionedlayer varying progressively from 0% at the surface of said iirst mentioned layer in contact with said second layer to at the'surface of said rst mentioned layer in contact with said third layer.

8. An electrically conductive transparent article comprising a body of transparent material having a smooth continuous surface, an electrically conductive continuous transparent layer on said smooth surface and carried by said body, said layer composed essentially of an intimate molecular mixture of metal and a metallic inorganic dielectric compound, in which said dielectric compound consists of a metal cation and at least one anion from the group consisting of bromine, chlorine, fluorine and iodine, the layer being substantially uniform in thickness, the proportion of metal to the dielectric compound in such layer and the thickness of said layer being such that said layer has substantial electrical conductivity and serves to carry the major portion of electrical cu-rrent carried by said article with the light transmission of the article being at least 50% and the other surface of said layer being substantially smooth.

9. An article as dened in claim 8, in which said metallic inorganic dielectric compound is magnesium iluoride.

10. An article as defined in claim 8, in which the metal is copper.

1l. An article as defined in claim 8, in which the metallic inorganic dielectric compound is magnesium uoride and said metal is copper.

12. An electrically conductive transparent article, comprising a body of transparent material, an electrically conductive continuous transparent layer carried by said body, said layer composed essentially of an intimate molecular mixture of a metal and a metallic inorganic dielectric compound, in which the dielectric compound consists of a metal cation and at least one anion from the group consisting of bromine, chlorine, fluorine and iodine, the layer being substantially uniform in thickness, the proportion of metal to the dielectric compound in such layer and the thickness of said layer being such that said layer has substantial electrical conductivity and serves to carry the major portion of electrical current carried by said article `with the light trans-mission of the article being at least 50% and the other surface of said layer being substantially smooth.

References Cited in the file of this patent UNITED STATES PATENTS 1,982,774 Winkler et al. Dec. 4, 1934 2,456,241 Axler et al Dec. 14, 1948 2,518,434 Lubszynski Aug. 8, 1950 2,586,752 Weber et al. Feb. 19, 1952 2,614,524 Haynes Oct. 21, 1952 2,628,921 Weinrich Feb. 17, 1953 2,628,927 Colbert et al. Feb. 17, 1953 2,808,351 Colbert et al. Oct. 1, 1957 

8. AN ELECTRICALLY CONDUCTIVE TRANSPARENT ARTICLE COMPRISING A BODY OF TRANSPARENT MATERIAL HAVING A SMOOTH CONTINUOUS SURFACE, AN ELECTRICALLY CONDUCTIVE CONTINUOUS TRANSPARENT LAYER ON SAID SMOOTH SURFACE AND CARRIED BY SAID BODY, SAID LAYER COMPOSED ESSENTIALLY OF AN INTIMATE MOLECULAR MIXTURE OF METAL AND A METALLIC INORGANIC DIELECTRIC COMPOUND, IN WHICH SAID DIELECTRIC COMPOUND CONSISTS OF A METAL CATION AND AT LEAST ONE ANION FRONT THE GROUP CONSISTING OF BROMINE, CHLORINE, FLUORINE AND IODINE, THE LAYER BEING SUBSTANTIALLY UNIFORM IN THICKNESS, THE PROPORTION OF METAL TO THE DIELECTRIC COMPOUND IN SUCH LAYER AND THE THICHNESS OF SAID LAYER BEING SUCH THAT SAID LAYER HAS SUBSTANTIAL ELECTRICAL CONDUCTIVITY AND SERVES TO CARRY THE MAJOR PORTION OF ELECTRIAL CURRENT CARRIED BY SAID ARTICLE WITH THE LIGHT TRANSMISSION OF THE ARTICLE BEING AT LEAST 50% AND THE OTHER SURFACE OF SAID LAYER BEING SUBSTANTIALLY SMOOTH. 